|Numéro de publication||US7616312 B2|
|Type de publication||Octroi|
|Numéro de demande||US 11/169,423|
|Date de publication||10 nov. 2009|
|Date de dépôt||29 juin 2005|
|Date de priorité||29 juin 2005|
|État de paiement des frais||Payé|
|Autre référence de publication||US20070002329|
|Numéro de publication||11169423, 169423, US 7616312 B2, US 7616312B2, US-B2-7616312, US7616312 B2, US7616312B2|
|Inventeurs||Steven Kasapi, Kenneth Wilsher, Gary Woods, William Lo, Radu Ispasoiu, Nagamani Nataraj, Nina Boiadjieva|
|Cessionnaire d'origine||Dcg Systems, Inc.|
|Exporter la citation||BiBTeX, EndNote, RefMan|
|Citations de brevets (53), Citations hors brevets (25), Référencé par (7), Classifications (5), Événements juridiques (4)|
|Liens externes: USPTO, Cession USPTO, Espacenet|
1. Field of the Invention
The present invention relates to an apparatus and method for probing integrated circuits using laser illumination.
2. Description of the Related Art
Probing systems have been used in the art for testing and debugging integrated circuit (IC) designs and layouts. Various laser-based systems for probing IC's are known in the prior art. While some description of the prior art is provided herein, the reader is encouraged to also review U.S. Pat. Nos. 5,208,648, 5,220,403 and 5,940,545, which are incorporated herein by reference in their entirety. Additional related information can be found in Soref, R. A. and B. R. Bennett, Electrooptical Effects in Silicon. IEEE Journal of Quantum Electronics, 1987. QE-23(1): p. 123-9; Kasapi, S., et al., Laser Beam Backside Probing of CMOS Integrated Circuits. Microelectronics Reliability, 1999. 39: p. 957; Wilsher, K., et al. Integrated Circuit Waveform Probing Using Optical Phase Shift Detection, in International Symposium for Testing and Failure Analysis (ISTFA), 2000, p 479-85; Heinrich, H. K., Picosecond Noninvasive Optical Detection of Internal Electrical Signals in Flip-Chip-Mounted Silicon Integrated Circuits. IBM Journal of Research and Development, 1990. 34(2/3): p. 162-72; Heinrich, H. K., D. M. Bloom, and B. R. Hemenway, Noninvasive sheet charge density probe for integrated silicon devices. Applied Physics Letters, 1986. 48(16): p. 1066-1068; Heinrich, H. K., D. M. Bloom, and B. R. Hemenway, Erratum to Noninvasive sheet charge density probe for integrated silicon devices. Applied Physics Letters, 1986. 48(26): p. 1811.; Heinrich, H. K., et al., Measurement of real-time digital signals in a silicon bipolar junction transistor using a noninvasive optical probe. IEEE Electron Device Letters, 1986. 22(12): p. 650-652; Hemenway, B. R., et al., Optical detection of charge modulation in silicon integrated circuits using a multimode laser-diode probe. IEEE Electron Device Letters, 1987. 8(8): p. 344-346; A. Black, C. Courville, G Schultheis, H. Heinrich, Optical Sampling of GHz Charge Density Modulation in Silicon Bipolar Junction Transistors Electronics Letters, 1987, Vol. 23, No. 15, p. 783-784, which are incorporated herein by reference in their entirety.
As is known, during debug and testing of an IC, a commercially available Automated Testing Equipment, also known as Automated Testing and Evaluation, (ATE) is used to generate test patterns (also referred to as vectors) to be applied to the device under test (DUT). When a laser-based probing system is used for the testing, the DUT is illuminated by the laser and the light reflected from the DUT is collected by the probing system. As the laser beam strikes the DUT, it is modulated by the response of various elements of the DUT to the vectors. This has been ascribed to the electrical modulation of the free carrier density and the resultant perturbation of the index of refraction of the material. Accordingly, analysis of the reflected light provides information about the operation of various devices on the DUT.
The various elements of probe system 100 will now be described in more detail. Since temporal resolution is of high importance in testing DUT's, the embodiment of
For probing the DUT 160, the ATE 140 sends stimulus signals 142 to the DUT, in synchronization with the phase-locked loop on the time-base board 155. In synchronization with the stimulus, the MLL 104 emits laser pulses that illuminate the particular device on the DUT that is being stimulated. The light is then reflected from the DUT, but the reflection changes character depending on the reaction of the device to the stimulus signal. The reflected light is then collected by the beam optics 125 and is transmitted to two photodetectors 136, 138 via fiber optic cables 132, 134. The output signal of the photodetectors 132, 134 is sent to signal acquisition board 150, which, in turn, sends the signal to the controller 170. Using the photodetectors signals and the synch signal from the time base board 155, the controller 170 can analyze the temporal response of the DUT. The temporal resolution of the analysis is dependent upon the width of the MLL pulse.
While the arrangement depicted in
A major difficulty encountered by all laser-base probe systems is deciphering the weak modulation in the reflected signal, which is caused by the response of the DUT to the stimulus. Another difficulty is noise introduced into the signal by the DUT's vibrations. Various beam manipulation optic, 135, designs have been used in the art in an attempt to solve these difficulties.
Since the DUT interaction with the laser beam causes change in the phase of the reflected beam, various phase detection schemes have been developed for the beam manipulation optics 135.
While this arrangement helps detect phase variations caused by the DUT, using this optical arrangement exposes the system to additional noise source from phase variations caused by DUT vibrations. The DUT vibrations still modulate reflected DUT beam amplitude, but now also modulate the DUT beam phase, which generates larger resultant reflected beam intensity modulations. Additional adjustments that are required in order to get best performance include reference arm power control and reference arm mirror position control (to set phase offset between DUT and Reference Arm powers). Also, alignment of reflected DUT and reference arm beams can be difficult.
As can be understood, various IC's have different layouts and different devices on the IC's have different dimensions. Therefore, using this embodiment for each new IC the user needs to decide where to place each beam for each test and each device to be tested within the chip. Moreover, since the beam needs to be placed at various locations on the chip, the system needs to be designed so that the beam separation is adjustable, which complicates the optics design. Additionally, the intensity ratio of the beams must be variable since the reflectivity of the regions where they are placed can differ. Power matching between the two beams is required for best results.
Experience with devices as depicted in
Accordingly, there is a need in the art for a system that will allow improved laser probing of a DUT, while simplifying operation and minimizing the system's complexity and cost.
Various embodiments of the present invention provide apparatus and method for laser probing of a DUT at very high temporal resolution, while enabling use of a conventional continuous wave (CW) laser source.
In one aspect of the invention, a system for probing a DUT is provided, the system comprising a CW laser source, a beam optics designed to point a reference beam and a probing beam at the same location on the DUT, optical detectors for detecting the reflected reference and probing beams, a collection electronics, and an oscilloscope.
In various illustrative implementations the beam optics comprise a common-path polarization differential probing (PDP) optics. The common-path PDP optics divides the laser beam into two beams of orthogonal polarization—one beam simulating a reference beam while the other simulating a probing beam. Both reference and probing beams are pointed to the same location on the DUT. Due to the intrinsic asymmetry of a CMOS transistor, the interaction of the reference and probing beams with the DUT result in different phase modulation in each beam. This difference can be investigated to study the response of the DUT to the stimulus signal.
Various embodiments of the invention also provide for a Laser Scanning Microscope (LSM) operable in a scanning mode and a vector-pointing mode. The scanning mode is used to obtain an image of an area of the DUT for navigation purposes, while the vector-pointing mode is used to park the beam on a specific device for probing.
In another embodiment of the invention, a system for testing an integrated circuit (IC) stimulated to simulate operating conditions is provided. The system includes a navigation light path and a probing light path. A first illumination source is used in the navigation mode to obtain an image of a specified area of the DUT via the navigation light path. Then, the light path is switched to the probing mode and a second light source is used to probe the DUT. The second light source may be a laser light source and the probing light path may include the common-path PDP optics. The probing light path may further include a solid immersion lens (SIL).
According to one aspect of the invention, a system for testing an integrated circuit microchip using laser probing is provided, which comprises a laser source providing a laser beam; a beam optics receiving said laser beam and providing a first and a second orthogonally polarized beams; a beam pointing optics receiving said first and second orthogonally polarized beams and pointing the first and second orthogonally polarized beams onto the same point on the microchip; a first photodetector receiving reflected laser light that is reflected from said microchip and providing an electrical signal; collection electronics receiving the electrical signal from said photodetector and providing an output signal; and an analysis system receiving and analyzing said output signal.
According to another aspect of the invention, a method of testing an integrated circuit microchip is provided, the method comprising generating a laser beam; transferring the laser beam through optical elements so as to obtain a reference beam polarized in one direction and a probing beam polarized in an orthogonal direction to the one direction; pointing the reference beam and the probing beam at a common selected area on the microchip; and collecting and analyzing reflected light that is reflected from the selected area.
According to yet another aspect of the invention, an interferometer system is provided, comprising a laser source providing a laser beam; a polarizer polarizing said laser beam in a first direction; a Faraday rotator rotating the beam to align said polarization in a second direction, so as to effectively produce a first polarized beam aligned in said first direction and a second polarized beam aligned in a third direction that is orthogonal to said first direction; an optical retarder, retarding one of the first and second polarized beams; and an objective lens directing said first and second polarized beams onto a common point on a specimen.
Other aspects and features of the invention will become apparent from the description of various embodiments described herein, and which come within the scope and spirit of the invention as claimed in the appended claims.
The invention is described herein with reference to particular embodiments thereof, which are exemplified in the drawings. It should be understood, however, that the various embodiments depicted in the drawings are only exemplary and may not limit the invention as defined in the appended claims.
An embodiment of the invention will now be described in details with reference to
In this particular embodiment, the laser beam is polarized in polarizer 604 and transferred to the beam optics 625 via fiber optics 615. Of course, free-space coupling can be used instead; however, if fiber optics coupling is used, it is expected to be polarization-maintaining fiber optics. Beam optics 625 needs to deliver the laser beam to selected points within the DUT. While any optical system for pointing a beam can be used, in this embodiment this is achieved by utilizing a Laser Scanning Microscope (LSM 630). An objective lens (not shown) is typically used to generate a focused spot in the DUT. The objective can be a normal air-gap objective, a liquid immersion objective, or a solid-immersion lens (SIL) objective.
In this embodiment beam optics 625 also includes a common-path polarization differential optics PDP 635. While other arrangement can be used, the common-path PDP 635 is expected to provide performance improvement and better ease-of-use compared to alternatives. The common-path PDP optics is described in more details below and its principle is illustrated in the broken-line circle in
Light reflected from the DUT is collected and applied to fiber optics 632, 634. As before, fiber coupling is optional and free-space coupling can also be used. If fibers are used, they can be single mode fiber, multimode fiber variety, for maximum coupling efficiency, or they may be fiber amplifier type, to provide optical gain so as to reduce electronic noise. Other optical amplifiers may also be used. The fiber optics 632, 634, deliver the reflected light to photodetectors 636, 638. The photodetectors can be any conventional light detectors, such as PIN diode, avalanche photo diode (APD), etc. For example, an InGaAs APD with 6 GHz bandwidth, conventionally used by the telecom industry, can be used. APD's have internal gain and can be used so as to reduce the overall system electronic noise. The internal gain of APD's can be changed by varying the applied reverse bias voltage. The output signal of the photodetectors 636, 638 is collected by receiver electronics 652, and the output of the receiver electronics 652 is applied to the oscilloscope 656.
Various embodiments of the receiver electronics 652 will be described below. On the other hand, the oscilloscope 656 may be a conventional off-the-shelf instrument, or may be replaced with other conventional testers such as, e.g., spectrum analyzer, edge discriminator (for jitter investigations), a lock-in amplifier, etc. For an improved ease-of-use, the oscilloscope 656 may be controlled by computer 670. Specifically, computer 670 can be programmed to enable better control by providing a simpler and programmable user interface. For optimal system performance the oscilloscope 656 should be chosen to have certain capabilities, such as high memory capacity and high memory access speed. In this embodiment, the oscilloscope's memory is segmented to provide enhanced capability.
The system of
During data acquisition operation, the laser beam is pointed to a particular point on the DUT, while the DUT is stimulated using various stimulus signals 642. When the test signal is applied to the illuminated device, the laser light reflected from that device is modulated by the reaction of the device to the stimulating signal. The reflected laser light is then collected and analyzed by the system. When the output signal obtained by the system is faint, the stimulus signal 642 should be designed to drive the DUT in a repetitive manner so as to obtain several measurements for each desired location/device, and the resulting measurements may be averaged. The signals 642 may be as simple as power and ground plus a test signal delivered via conventional probes (not shown). Of course, for more complex ICs and more elaborate testing, an ATE tester 140 can be used to deliver complex and programmable signals 642, or the DUT can be running test signals internally and independently. Regardless of the stimulus applied, a trigger signal 644 may also be provided to synchronize the oscilloscope 656, depending on the information sought. For example, if the DUT is being tested for temporal response to the stimulating signal, then a synchronizing signal should be provided to the oscilloscope. However, for other investigations, e.g., when a spectrum analyzer is used, no synchronization signal is needed.
The optical bench 612 may include a conventional vibration isolation system (not shown) to isolate the DUT 660 and the beam optics 625 from ambient or vibrations noise or mechanical noise generated by the DUT stimulus. The use of vibration isolation system may be avoided by proper optical system design. The goal is to minimize unwanted movement of the DUT 660 relative to the beam optics 625 during imaging and signal acquisition. Relative movement can cause return laser intensity variations (due to defocusing effects, for example) that degrade the signal to noise ratio (SNR) of the measurement and degrade image quality.
As can be understood, the inventive system is advantageous over the prior art system in that it uses mostly inexpensive and conventionally available components in an arrangement that produces superior results to prior systems using specifically designed components. For example, the described embodiment uses a CW laser source, rather than the complex mode-locked laser source. Similarly, a commercially available oscilloscope can be used, rather than complex and custom high-speed timing electronics. The light detectors can be InGaAs APD's which are conventionally used by the telecom industry. Additionally, the common-path PDP optics provides ease-of-use benefits over previous schemes, especially since both the reference and probing beams are aimed at the same location. The common-path PDP optics also reduces the sensitivity of the system to vibrations, as both the reference and probing beams traverse the identical path.
The image obtained can be used for navigation and correct placement of the laser beam for probing. That is, depending on the particular test to be run, one may wish to select any particular section or device on the DUT for laser probing. Using information about the chip design and layout stored in CAD software 780′, such as, for example, Cadence™, and using navigation software 780′, such as, for example, Merlin's Framework™ available from Knights Technology (www.electroglass.com), one may select a particular device for any particular test and use computer 780 to place the beam at the correct location for the test.
To switch to laser probing mode, mirrors 735 and 765 are flipped into the position illustrated in solid lines. In this position light source 730 is turned off and laser source 740 is turned on. Light from laser source 740 is deflected by mirrors 765 and 760, so as to enter beam optics 720. Beam optics 720 may be a common-path PDP optics as described herein. Additionally, in this arrangement an optional solid immersion lens (SIL) 790 is added to the beam optics 720. SIL 790 may be any conventional solid immersion lens and may be used in conjunction with index matching fluid. The laser beam is reflected by the DUT and the reflection is collected by the beam optics 720, deflected by mirrors 760 and 735, and detected by detector 750. As explained before, the reflected light is modulated by the DUT according to its response to the test signals. The output of the detector 750 is collected by the electronics 755 and sent to computer 780. For that purpose, electronics 755 includes the necessary elements as described herein, such as, e.g., differential amplifier, balanced receiver, spectrum analyzer, oscilloscope, edge analyzer, etc. The utilization of these elements will depend on the application. Additionally, as with the other embodiments described herein, if temporal resolution is needed, a synchronization signal may also be provided from the test signal generating equipment.
The beam from the laser source enters the first polarizing beam splitter PBS1 so that part of the beam is deflected towards light sensor 1010. The output of the sensor 1010 is used to monitor the beam's intensity and is not part of the PDP optics, but rather an optional intensity monitor. The remaining part of the beam that passes through the first PBS cube (PBS1) enters the second polarizing beam splitters PBS2, which is oriented to pass only a vertically oriented beam. The beam's polarization state is rotated 45 degrees from the vertical by the action of the Faraday rotator (FR) and the third PBS cube (PBS3) is oriented to transmit the rotated beam. Consequently, at this stage the beam is the equivalent of superposition of a vertically polarized beam and a horizontally polarized beam, both beams equal in amplitude and in phase with each other. The dotted circles in the incident beam path, between PBS3 and VR, indicate the equivalence between a 45-degree polarized beam and two in-phase, equal amplitude beams that are polarized vertically and horizontally.
The two beams then enter the variable retarder VR. The fast and slow axes of the variable-retarder (VR) are aligned along these two vertical and horizontal polarization directions. Thus, after passage through the VR, the beam consists of two spatially coincident, equal-amplitude, orthogonally polarized beams that are phase-shifted (retarded) with respect to each other by a small amount (nominally, π/4). This is indicated in the illustration by the dot being slightly behind the vertical arrow. The two beams are then focused onto the same point on the DUT by the objective lens OL. The DUT is oriented such that the polarization directions of these two beams are aligned with the length and width directions of the transistor gates. Interaction with the DUT phase modulates one of the beams relative to the other by a small amount. In this manner, the beam being modulated by the DUT may be thought of as the probing beam, while the other beam may be thought of as the reference beam. Of course, unlike prior art interferometers, here none of the beams traverses a reference optical path, but rather both beams traverse the identical path to the probing location. Therefore, in this sense, there is not reference beam and probing beam, but for convenience one may refer to one beam as the reference beam and the other as the probing beam.
After the beams are reflected by the DUT (
As can be understood, since both reference and probing beams are pointed to the same location on the DUT, it means that this scheme has better phase noise immunity then prior art interferometric systems. Additionally, there is no need to find a second location for the reference beam for each location tested. Rather, both beams are always pointed at the location to be tested. Accordingly, there is also no need to introduce separate spatial control of the reference and probing beams. Consequently, the inventive common-path PDP arrangement can be used in multiple applications where phase interferometry is needed.
On the other hand,
In any of the disclosed embodiments, it is advantageous to make the cutoff of the amplifier low, otherwise the low frequency component of the signal of interest would be almost completely attenuated. In an ideal situation, to capture the signal with good fidelity the response of the amplifier should extend down in frequency to the DC. However, in practice the reflected beam will carry a low frequency noise, mostly at about 10-200 Hz, due to DUT vibrations relative to the incident beam. The noise introduced by the DUT vibration can be very large as compared to the beam modulation, which is the signal of interest. Therefore, a cutoff in the amplifier's response should be introduced so as to remove this noise. The cutoff may be set at, say 100 KHz or below.
The signal from APD 1340 is applied to amplifier 1320, while the signal from APD 1350 is applied to amplifier 1310. The output of both amplifiers are applied to a simple resistive summing junction 1330 to effectively add the two APD signals together and provide a probing signal Vout. The probing signal is sent to a digitizer for data storage and processing. In this embodiment filters 1345 and 1355 have been introduced to remove vibration and other noise appearing at below about 2 KHz.
During navigation, signal from only one APD is required to obtain an image of the DUT. As is shown, the signal from APD 1340 is also sent to amplifier 1360 and therefrom to video amplifier 1370, which provides a video out signal for processing and display. Other imaging methods may be performed with the resulting advantageous features as follows. In order to provide contrast control, the variable retarder may be varied to tune the retardation so that the image contrast is varied to the desired result. Additionally, imaging may be performed using both APD's and the resulting images subtracted from each other so as to obtain a difference image.
In the various embodiments disclosed where two APD's are used, the APD's gain may be advantageously controlled to, first, balance the APD's response and, second, to improve the imaging. Using a controllable variable power supply that is manually or automatically controlled, the voltage/gain response of each APD can be determined. Then, using the learned voltage/gain response, the gain of each APD can be controlled to a desired value by selecting the appropriate voltage on the corresponding power supply. For balancing the system, the following procedure may be used. First, the voltage of the power supplies of each APD is set to result in the same gain provided by both APD's, thereby balancing the output of the APD's. Then, the variable wave plate is adjusted until the current output of both ADP's is the same, thereby balancing the optical path. The variable gain can also be used for improved imaging. For example, when the image scan goes from a relatively dark area to a relatively bright area, the gain of the APD's may be reduced so as not to saturate the image. Conversely, when moving from a bright area to a dark area, the gain may be increased to provide improved contrast and detail.
As can be understood from the above description, the common-path PDP optics provides a reference and probing optical paths that are inherently of the same length. However, when two detectors are used for differential probing, some path length difference may be introduced by the fiber optics and the other optical elements.
The fiber collimator module includes a collimator lens 1550, which receives the fiber output beam 1505 and collimates it. The collimated light is directed towards the focusing lens 1555 using x-y alignment screws 1510. Since the light between the collimating lens 1550 and focusing lens 1555 is collimated, changing the separation between these lenses, i.e., distance D, will not cause degradation or changes in the optical signal. Therefore, changing this distance, e.g., by alignment screws 1510, enables matching the optical path of each beam to balance the reference and probing beams. An alignment O-ring 1515 assists in maintaining the fiber collimator module in the tuned position once balance is achieved.
While the invention has been described with reference to particular embodiments thereof, it is not limited to those embodiments. Specifically, various variations and modifications may be implemented by those of ordinary skill in the art without departing from the invention's spirit and scope, as defined by the appended claims. Additionally, all of the above-cited prior art references are incorporated herein by reference.
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|Classification aux États-Unis||356/369|
|Classification coopérative||G01R31/308, G01R31/311|
|3 oct. 2005||AS||Assignment|
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Owner name: DCG SYSTEMS, INC., CALIFORNIA
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